The 'thin-wall approximation' gives a simple estimate of the decay rate of an
unstable quantum field. Unfortunately, the approximation is uncontrolled. In
this paper I show that there are actually two different thin-wall
approximations and that they bracket the true decay rate: I prove that one is
an upper bound and the other a lower bound. In the thin-wall limit, the two
approximations converge. In the presence of gravity, a generalization of this
lemma provides a simple sufficient condition for non-perturbative vacuum
instability.Comment: technically contains 2 lemma